Boolean Functions
Introduction
Let π½2π be the vector space of dimension π over the finite field with two elements. The vector space can also be endowed with the structure of the field, the finite field with 2π elements, π½2π. A function [math]\displaystyle{ f : \mathbb{F}_2^n\rightarrow\mathbb{F} }[/math] is called a Boolean function in dimenstion π (or π-variable Boolean function).
Given [math]\displaystyle{ x=(x_1,\ldots,x_n)\in\mathbb{F}_2^n }[/math], the support of x is the set [math]\displaystyle{ supp_x=\{i\in\{1,\ldots,n\} : x_i=1 \} }[/math]. The Hamming weight of π₯ is the size of its support ([math]\displaystyle{ w_H(x)=|supp_x| }[/math]). Similarly the Hamming weight of a Boolean function π is the size of its support, i.e. the set [math]\displaystyle{ \{x\in\mathbb{F}_2^n : f(x)\ne0 \} }[/math]. The Hamming distance of two functions π,π is the size of the set [math]\displaystyle{ \{x\in\mathbb{F}_2^n : f(x)\neq g(x) \}\ (w_H(f\oplus g)) }[/math].
Representation of a Boolean function
There exist different ways to represent a Boolean function. A simple, but often not efficient, one is by its truth-table. For example consider the following truth-table for a 3-variable Boolean function π.
π₯ | π(π₯) | ||
---|---|---|---|
0 | 0 | 0 | 0 |
0 | 0 | 1 | 1 |
0 | 1 | 0 | 0 |
0 | 1 | 1 | 0 |
1 | 0 | 0 | 0 |
1 | 0 | 1 | 1 |
1 | 1 | 0 | 0 |
1 | 1 | 1 | 1 |
Algebraic normal form
An π-variable Boolean function can be represented by a multivariate polynomial over π½2 of the form
Such representation is unique and it is the algebraic normal form of π (shortly ANF).
The degree of the ANF is called the algebraic degree of the function, πΒ°π=max { |πΌ| : ππΌβ 0 }.
Based on the algebraic degree we called π
- affine if πΒ°π=1, linear if πΒ°π=1 and π(π)=0;
- quadratic if πΒ°π=2.
Affine functions are of the form π(π₯)= π’β π₯+π, for π’βπ½2π and πβπ½2
Trace representation
We identify the vector space with the finite field and we consider π an π-variable Boolean function of even weight (hence of algebraic degree at most π-1). The map admits a uinque representation as a univariate polynomial of the form
with Ξπ set of integers obtained by choosing one element in each cyclotomic coset of 2 ( mod 2π-1), π°(π«) size of the cyclotomic coset containing π«, ππ« β π½2π°(π«), Trπ½2π°(π«)/π½2 trace function from π½2π°(π«) to π½2.
Such representation is also called the univariate representation .
π can also be simply presented in the form [math]\displaystyle{ \mbox{Tr}_{\mathbb{F}_{2^n}/\mathbb{F}_2}(P(x)) }[/math] where π is a polynomial over the finite field F2π but such representation is not unique, unless π°(π«)=π for every π« such that ππ«β 0.
When we consider the trace representation of of a function, then the algebraic degree is given by [math]\displaystyle{ \max_{j\in\Gamma_n | A_j\ne0}w_2(j) }[/math], where π2(π) is the Hamming weight of the binary expansion of π.
The Walsh transform
The Walsh transform ππ is the descrete Fourier transform of the sign function of π, i.e. (-1)π(π₯). With an innner product in π½2π π₯Β·π¦, the value of ππ at π’βπ½2π is the following sum (over the integers)
The set [math]\displaystyle{ \{ u\in\mathbb{F}_2^n : W_f(u)\ne0 \} }[/math] is the Walsh support of π.
Properties of the Walsh transform
For every π-variable Boolean function π we have the following relations.
- Inverse Walsh transform: for any element π₯ of π½2π we have
[math]\displaystyle{ \sum_{u\in\mathbb{F}_2^n}W_f(u)(-1)^{u\cdot x}= 2^n(-1)^{f(x)}; }[/math] - Parseval's relation:
[math]\displaystyle{ \sum_{u\in\mathbb{F}_2^n}W_f^2(u)=2^{2n}; }[/math] - Poisson summation formula: for any vector subspace πΈ of π½2π and for any elements π,π in π½2π
[math]\displaystyle{ \sum_{u\in a+E^\perp}(-1)^{b\cdot u}W_f(u) = |E^\perp|(-1)^{a\cdot b}\sum_{x\in b+E}(-1)^{f(x)+a\cdot x}, }[/math] for πΈβ the orthogonal subspace of πΈ,{π’βπ½2π : π’Β·π₯=0, for all π₯βπΈ}.
Equivalence of Boolean functions
Two π-variable Boolean functions π,π are called extended-affine equivalent (shortly EA-equivalent) if there exists a linear automorphism πΏ, an affine Boolean function π and a vecor π such that
A parameter that is preserved by EA-equivalence is called EA-invariant.